Method of fast surface particle and scratch detection for euv mask backside

ABSTRACT

A method of scanning a substrate and determining scratches of the substrate includes transmitting a converging beam of light that comprises multiple wavelengths to the substrate. Each wavelength of the multiple wavelengths focuses at a different distance in a focus interval around and including a surface of the substrate. The method also includes receiving reflected light from the surface of the substrate and determining a height or depth of the surface of the substrate based on a wavelength of the reflected light a highest intensity.

PRIORITY CLAIM AND CROSS-REFERENCE

This application is a continuation of U.S. patent application Ser. No.17/094,727 filed on Nov. 10, 2020, which claims priority to U.S.Provisional Application No. 62/955,846 filed on Dec. 31, 2019, entitled“Method of Fast Surface Particle and Scratch Detection for EUV MaskBackside,” the entire disclosure of which is incorporated herein byreference.

BACKGROUND

During an integrated circuit (IC) design, a number of layout patterns ofthe IC, for different steps of IC processing, are generated. The layoutpatterns include geometric shapes corresponding to structures to befabricated on a wafer. The layout patterns may be produced byprojecting, e.g., imaging, a mask on the wafer. The mask includes alayout pattern that is produced on a clean (with no pattern)semiconductor substrate or a mask blank. Thus, the masks include alayout pattern of the IC or a layout pattern of a portion of the IC thatis created on the mask blank. A lithography process transfers a layoutpattern of the mask to the wafer such that etching, implantation, orother steps are applied only to predefined regions of the wafer.

In some embodiments, a reflective mask is used during extremeultraviolet (EUV) lithography process to form an integrated circuithaving smaller feature sizes. Reflective masks are vulnerable tomanufacturing/fabrication defects, such as oxidation and particles, andare easily damaged. Therefore, a number of defects may exist on the masksurface that can affect the layout printing that are produced bypatterned masks. In addition, the printing error of the layout patternof the mask may impact the fabricated circuit on the wafer. An efficientmask blank scanning (e.g., mapping) is desirable to detect the defect ofthe mask blank to avoid the impact of the defects when producing themask on the mask blank.

In some embodiments, a scratch is on the backside including the backsideedge of the mask and the scratch causes defects such as dips or bumps onthe front side of the mask or causes a defect, e.g., anomaly, in thethickness of the mask that is desirable to be avoided. Therefore, thebackside including the backside edges of the mask blank is scanned(e.g., mapped) for the scratches to determine areas of the maskincluding edge zones of the mask that is desirable to be avoided whenthe mask is created on the mask blank.

BRIEF DESCRIPTION OF THE DRAWING

The present disclosure is best understood from the following detaileddescription when read with the accompanying figures. It is emphasizedthat, in accordance with the standard practice in the industry, variousfeatures are not drawn to scale and are used for illustration purposesonly. In fact, the dimensions of the various features may be arbitrarilyincreased or reduced for clarity of discussion.

FIGS. 1A and 1B illustrate optical scanning systems for scanning asubstrate in accordance with some embodiments of the present disclosure.

FIG. 2 illustrates an optical scanning system for scanning a substratein accordance with some embodiments of the present disclosure.

FIG. 3 illustrates an optical scanning system for scanning a substratein accordance with some embodiments of the present disclosure.

FIGS. 4A and 4B illustrate substrates that include scratches inaccordance with some embodiments of the present disclosure.

FIG. 5 illustrates a detector system for the optical scanning system inaccordance with some embodiments of the present disclosure.

FIGS. 6A and 6B illustrate line scans through the substrates of FIG. 4Athat include scratches and particle in accordance with some embodimentsof the present disclosure.

FIGS. 7A and 7B illustrate line scans through the substrates of FIG. 4Bthat include scratches and particles in accordance with some embodimentsof the present disclosure.

FIG. 8 illustrates an exemplary optical scanning system for scanning asubstrate and determining scratches of a substrate in accordance withsome embodiments of the disclosure.

FIG. 9 illustrates a flow diagram of an exemplary process for scanning asubstrate and determining scratches of the substrate in accordance withsome embodiments of the disclosure.

FIGS. 10A and 10B illustrate an apparatus for scanning a substrate anddetermining scratches of the substrate in accordance with someembodiments of the disclosure.

DETAILED DESCRIPTION

The following disclosure provides many different embodiments, orexamples, for implementing different features of the provided subjectmatter. Specific examples of components and arrangements are describedbelow to simplify the present disclosure. These are, of course, merelyexamples and are not intended to be limiting. For example, the formationof a first feature over or on a second feature in the description thatfollows may include embodiments in which the first and second featuresare formed in direct contact, and may also include embodiments in whichadditional features may be formed between the first and second features,such that the first and second features may not be in direct contact. Inaddition, the present disclosure may repeat reference numerals and/orletters in the various examples. This repetition is for the purpose ofsimplicity and clarity and does not in itself dictate a relationshipbetween the various embodiments and/or configurations discussed.

Further, spatially relative terms, such as “beneath,” “below,” “lower,”“above,” “upper” and the like, may be used herein for ease ofdescription to describe one element or feature's relationship to anotherelement(s) or feature(s) as illustrated in the figures. The spatiallyrelative terms are intended to encompass different orientations of thedevice in use or operation in addition to the orientation depicted inthe figures. The apparatus may be otherwise oriented (rotated 90 degreesor at other orientations) and the spatially relative descriptors usedherein may likewise be interpreted accordingly. In addition, the term“being made of” may mean either “comprising” or “consisting of.” In thepresent disclosure, a phrase “one of A, B and C” means “A, B and/or C”(A, B, C, A and B, A and C, B and C, or A, B and C), and does not meanone element from A, one element from B and one element from C, unlessotherwise described.

In some embodiments, a substrate, e.g., a mask blank, is scanned forbumps and dips. When producing a mask and imaging a layout pattern onthe mask blank, the bumps and dips are avoided for wafer printing errorconcerns. In some embodiments, a scratch on the backside of the maskblank causes dips and/or bumps on the front side of the mask blank wherethe layout pattern is created. In some embodiments, the scratch on thebackside of the mask blank causes some changes in the thickness of themask blank that although may not be visible on the front side of themask blank, may degrade the wafer layout pattern that is produced by themask. Therefore, the backside of the mask blank is examined forscratches and particles, e.g., bump and/or dips, and the areas of themask blank to be avoided, cleaned, or repaired is mapped. A fastscanning method for inspecting the backside of the mask blank isdesirable. In some embodiments, an edge region of the mask blank aremore vulnerable for having scratches or particles and thus the edgeregion of the mask blank is inspected. In some embodiments, the entirebackside of the mask blank is inspected.

In some embodiments, an optical system is used for scanning the backsideof the mask blank. The optical system has a multi-wavelength lightsource, e.g., a white light source, and a chromatic lens. The chromaticlens that may include a plurality of lenses, stacked together in series,creates a focal distance for each wavelength of the light source. Thus,when a collimated beam of light is transmitted to the chromatic lens,each component of the collimated beam of light having a differentwavelength is focused at a different focal point from the chromaticlens. In some embodiments, a component of the collimated beam of lighthaving a shorter wavelength has a shorter focal point and focuses closerto the chromatic lens than a component of the collimated beam of lighthaving a longer wavelength. Thus, for a collimated beam of white light,the violet component of the white light focuses closer to the chromaticlens than the green component and the green component focuses closer tothe chromatic lens than the red component of the white light.

In some embodiments, the collimated beam of light is focused on asubstrate. In some embodiments, the substrate has roughness with bumpsand dips. Thus, when the collimated beam of white light is focused onthe substrate, depending on the height of a bump or depth of a dip, adifferent color of the components of the white light is focused to apoint on the substrate and the other components are not focused andcreate a blurred and expanded points, e.g., spot, on the substrate. Insome embodiments, the reflected light from the substrate goes backthrough the chromatic lens and then is deflected by a mirror, e.g., abeam splitter, and the reflected and then deflected light is imaged to apinhole in a plane. The component of the multi-wavelength light that isin-focus on the substrate is thus imaged as a point on the pinhole andpasses, e.g., essentially entirely passes, through the pinhole and theother components of the white light that are not in-focus on thesubstrate are imaged as blurred and expanded points, e.g., spots, on thepinhole and, thus, only a fraction of the other components of the whitelight passes through the pinhole.

In some embodiments, the components of the white light or anymulti-wavelength light source, after passing through the pinhole passthrough a focusing lens of a spectrometer and then are detected perwavelength by the detectors of the spectrometer. In some embodiments,the spectrometer creates an output signal that is an intensity of thereflected light that passes through the pinhole as a function of thewavelength of the light. As noted, the component of the light thatfocuses on the substrate also focuses on the pinhole. Thus, if theoutput signal of the spectrometer passes through a peak detector, awavelength of the light having the peak intensity, e.g., having thehighest intensity, is determined. The wavelength of the light having thepeak intensity is the wavelength of the light that is in-focus on thesubstrate. As described, each component of the light source that has adifferent wavelength focuses at a different distance from the chromaticlens. Thus, the wavelength that focuses on the substrate may determinethe height or depth of the surface of the substrate. Therefore, thewavelength corresponding to the peak intensity of the output signal ofthe spectrometer determines the height of the surface of the substratein some embodiments.

FIGS. 1A and 1B illustrate optical scanning systems 100 and 180 forscanning a substrate in accordance with some embodiments of the presentdisclosure. The optical scanning system 100 of FIG. 1A includes a lightsource 116 and a light source controller 135 for controlling the lightsource 116. The light source controller 135 commands the light source116 to transmit a beam of light 134 that includes multiple wavelengthsto an optical device 114. The optical device 114 that is controlled byan optical controller 118 receives the beam of light 134 and in responsetransmits beams of light 142, 144, and 146 to a surface 131 of asubstrate 130. In some embodiments, the substrate 130 is a mask blankfor EUV lithography. In other embodiments, the substrate 130 is a maskblank for DUV lithography, a glass substrate, or a semiconductorsubstrate. As shown in FIG. 1A, the beams of light 142, 144, and 146focuses, e.g., converges, at different distances from the surface 131 ofthe substrate 130 such that the beam of light 142 focuses, e.g.,converges, at point A before the surface 131 of the substrate 130 (i.e.,the converging point is between the optical device 114 and the surface131). The beam of light 144 focuses, e.g., converges, at point B beforethe surface 131 of the substrate 130 and the beam of light 146 isconverging to point C after, e.g., under, the surface 131 of thesubstrate 130 (i.e., focus point is in the substrate 130). In someembodiments, when there is a bump 132 on the surface of the substrate130, the beam of light 144 focuses at the point A that is on the bump132 and thus the beam of light 144 converges as the point A on the bump132. The beam of light 142 that converges at the point A, generates aspot on the surface 131 of the substrate 130 that covers the bump 132and portions of the surface 131 of the substrate 130 in someembodiments. The beam of light 146 that would be converging to point Cafter the surface 131 of the substrate 130 also generates a spot on thebump 132. As noted, the beam of light 146 is stopped by a top surface ofthe bump 132 and, thus, the extensions of the beam of light 146 insidethe bump 132 and inside the substrate 130 is shown by broken lines 146B.In some embodiments, the optical controller 118 controls the lightsource 116 and commands the light source 116, via the light sourcecontroller 135, to transmit the beam of light 134.

In some embodiments, the substrate 130 is a mask blank that is placed ona stage 112 and the stage 112 is moved by a stage controller 110 suchthat the beam of light 134 is transmitted to multiple locations on thesurface of the substrate 130 and a line on the surface 131 of thesubstrate 130 or an area of the surface 131 of the substrate 130 isscanned, e.g., mapped. In some embodiments, the optical device 114receives the reflected light from the surface of the substrate 130 andtransmits, e.g., images, the reflected light from the surface 131 of thesubstrate 130 to a pinhole structure 124 that includes a pinhole 149. Insome embodiments, a position and a size of the pinhole 149 is controlledby the optical controller 118 such that a beam from the beams of light142, 144, and 146 that is in-focus on the surface of the substrate 130is also in-focus on the pinhole and substantially entirely, e.g., morethan 90 percent, passes through the pinhole 149 but the other beams oflight that are not in-focus on the surface 131 of the substrate 130 arenot also in-focus on the pinhole 149 and only a small fraction, e.g.,less than 30 percent, of the other beams of light pass through thepinhole 149. Thus, the optical controller 118 may adjust a distance 117between the pinhole structure 124 and the optical device 114 such thatthe reflected light from the surface of the substrate 130 is imaged onthe pinhole structure 124. In some embodiments, the optical controller118 moves the pinhole structure 124 and/or the optical device 114 toadjust the distance 117. In some embodiments, the optical device 114 isdesigned such that the reflected light from the beam of light that isfocused on the surface of the substrate is focused on the pinhole 149.The reflected light from the other beams of light that are not focusedon the surface of the substrate do not focus on the pinhole 149.

In some embodiments, the beam of light 142 has a wavelength w1, the beamof light 144 has a wavelength w2 (e.g., w2 greater than w1), and thebeam of light 146 has a wavelength w3 (e.g., w3 greater than w2). Insome embodiments, the stage controller 110 generates the location 158 ofthe surface 131 of the substrate 130 that is illuminated by the beams oflight 142, 144, and 146. Thus, the location 158 of the surface 131 is alocation that one the beams of light 142, 144, or 146 is in-focus. Insome embodiments, either the stage controller 110 moves the stage 112 upor down, or the optical controller 118 moves the optical device 114 upor down to adjust a distance 136 between the optical device 114 and thesubstrate 130 such that a beam of light with a specific wavelengthfocuses on the surface 131 of the substrate 130. In some embodiments,the beam of light 134 is a beam of light that includes a continuousspectrum of wavelengths and thus the wavelength w1, w2, and w3 areexamples of wavelengths in the beam of light 134. In some embodiments,the beam of light 134 is a white beam of light that includes acontinuous spectrum of wavelengths from red to green and thus thewavelength w1, w2, and w3 are examples of wavelengths such as violet,green, or red. In some embodiments, the surface 131 of the substrate 130is a backside surface of the substrate 130.

As shown in FIG. 1A, the beam of light 144 is in-focus on the bump 132and the reflected light from the bump 132 is also focused at the pinhole149 of the pinhole structure 124 and thus entirely, e.g., more than 90percent, passes through the pinhole 149. The reflected light from theother beams of light 142 and 146 that are not in-focus on the surface ofthe substrate 130 are not also focused at the pinhole structure 124.Thus, only a fraction, e.g., a small fraction less than 30 percent, ofthe reflected light from the other beams of light 142 and 146 passthrough the pinhole 149.

As noted, in some embodiments, the light source 116 is a white lightsource that includes wavelengths of the white light spectrum from red toviolet. In some embodiments, the beams of light 142, 144, or 146 havingthe longer wavelength focuses farther from the optical device 114 andthe beams of light 142, 144, or 146 having the shorter wavelengthfocuses closer to the optical device 114. Thus, when the light source116 is a white light source, the violet beam of light 142 having thewavelength w1 focuses above the surface 131 of the substrate 130 and thered beam of light 146 having the wavelength w3 may focus farther insidethe substrate 130 after, e.g., under, the surface 131 and the green beamof light 144 having the wavelength w2 focuses slightly above the surface131 of the substrate 130, e.g., about 10 micron above the surface 131between where the violet beam of light 142 and the red beam of light 146focus. In some embodiments, the light source 116 includes a continuousspectrum of color sources, e.g., between red and violet, which producethe white light.

In some embodiments, the beams of light that passes through the pinhole149 is imaged with a lens 122 on one or more light detectors 121 of aspectrometer 120. As shown in FIG. 1A, the reflected light that isfocused on the pinhole structure 124 entirely passes through the pinhole149 and thus produces a peak intensity in the light detectors 121. Asshown, the beam of light 144 (having the wavelength w2) that focuses onthe bump 132 of the substrate also focuses at the pinhole 149 andcreates the peak intensity in the spectrometer. In some embodiments, thelight source 116 includes multiple wavelengths and each light detector121 of the spectrometer 120, detects the received light intensity in aspecific wavelength, e.g., a specific short range of wavelengths. Thuseach one of the light detectors 121 detects one of the wavelengths ofthe multiple wavelengths and thus creates an intensity 141 versuswavelength 143 curve, a spectrum 148 of the detected light on a displayscreen 140. In some embodiments, the spectrometer 120 includes a prism(not shown) for splitting the direction of transmission of the multiplewavelengths and thus leading each wavelength, e.g., a short wavelengthrange, to one of the light detectors 121. As shown in FIG. 1A, thespectrometer 120 generates a spectrum data 152, which includes intensity141 per wavelength 143 of the received beams of light by the lens 122and detected by the light detectors 121. In some embodiments, a displaycontroller 115 receives the spectrum data 152 and displays the spectrumdata 152 on the display screen 140.

In some embodiments, a peak-wavelength detector 125 determines, e.g.,calculates or detects, the peak intensity of the spectrum 148 anddetermines a wavelength 154 corresponding to the peak intensity. Asnoted each wavelength of the multiple wavelengths of the beam of light134 converges at a specific distance from the optical device 114. Thus,in some embodiments, a height variation of the substrate, e.g., a height145 of the bump 132 on the substrate 130 is determined based on thewavelength of the light that converged, e.g., focused, on the bump 132and thus produced the peak intensity in the spectrum data 152. In someembodiments, a wavelength-to-height converter 126 receives thewavelength 154 corresponding to the peak intensity and generates aheight 156. For example, if the peak intensity is at w2 wavelength(e.g., in the green color range), the defect is a bump with a height 156of about 10 microns and if the peak intensity is at w3 wavelength (e.g.,in the red color range), the defect is a dip with a height 156 of −5microns (e.g., a depth of about 5 microns).

As shown in FIG. 1A, the beam of light 144 that has the wavelength w2focuses on the substrate 130, e.g., on the bump 132 of the substrate130. In addition, the deflected beam of light 144 impinging on thepinhole structure 124 also focuses on the pinhole structure 124 and thusentirely passes through the pinhole 149 and thus produces a peakintensity in the light detectors 121. Also, the spectrum 148 produces apeak at the wavelength w2 of the beam of light 144.

In some embodiments, the multi-wavelength of the light source 116includes one or more wavelength corresponding to desired heights anddepths of the defects. In some embodiments, the reflected light thatgoes through the pinhole 149 is filtered by the spectrometer to selectone or more wavelengths corresponding to defects having one or moredesired height or depth.

The optical scanning system 180 of FIG. 1B is consistent with theoptical scanning system of FIG. 1A with the difference that thespectrometer 120 of the optical scanning system 180 in addition to thelight detectors 121 includes the peak-wavelength detector 125 andwavelength-to-height converter 126. Also, the optical scanning system180 includes an optical system 185. In some embodiments, the opticalsystem 185 includes the optical device 114 of FIG. 1A and transmits thebeams of light 142, 144, and 146 to the surface of the substrate 130.

In addition, the optical system 185 receives the light reflected fromthe beams of light 142, 144, and 146 from the surface of the substrate130 and directs the reflected light from the beam of light that isfocused on the surface of the substrate out of an exit pupil 187 of theoptical system 185. In some embodiments, the optical system 185 includesthe pinhole 149. The optical system 185 is designed such that thereflected light from the beam of light that is focused on the surface ofthe substrate is focused on the pinhole 149 and thus transmits the lightthrough the pinhole. However, the reflected light from the other beamsof light that are not focused on the surface of the substrate do notfocus on the pinhole 149 and only a fraction of them transmits throughthe pinhole 149. In some embodiments, the optical system 185 is designedsuch that the reflected light from the beam of light that is focused onthe surface of the substrate transmits through the exit pupil 187 out ofthe optical system 185. The reflected light from the other beams oflight that are not focused on the surface of the substrate are nottransmitted through the exit pupil 187 out of the optical system 185. Asshown in FIG. 1B, the beam of light 144 focuses on the surface of thesubstrate 130 and thus the reflected light from the beam of light 144 istransmitted through the exit pupil 187 out of the optical system 185.

FIG. 2 illustrates an optical scanning system 200 for scanning asubstrate in accordance with some embodiments of the present disclosure.FIG. 2 , is consistent with FIG. 1A. The optical scanning system 200shows that the optical device 114 includes a chromatic lens 150 thatcreates the beams of light 142, 144, and 146 from the multi-wavelengthbeam of light 134. FIG. 2 also shows that the optical device 114includes a beam splitter 160. In some embodiments, a portion of the beamof light 134 passes through the beam splitter 160 and hits the chromaticlens 150 to create the beams of light 142, 144, and 146. The reflectedlight from the surface of the substrate is transmitted back through thechromatic lens 150 and is deflected by the beam splitter 160 to thepinhole structure 124. In some embodiments, the chromatic lens 150 andthe beam splitter 160 are used to image an illuminated surface 131 ofthe substrate 130 onto the pinhole structure 124.

FIG. 3 illustrates an optical scanning system 300 for scanning asubstrate in accordance with some embodiments of the present disclosure.FIG. 3 is consistent with FIG. 1A. As shown in FIG. 3 , the reflectedlight that is focused on the pinhole structure 124, e.g., the beam oflight 146, entirely passes through the pinhole 149 and thus produces apeak intensity in the light detectors 121. As shown, the beam of light146 (having the wavelength w3) that focuses at a bottom of a dip 133 onthe substrate 130 also focuses at the pinhole 149 and creates the peakintensity of the spectrometer 120. In some embodiments as described, thelight detectors 121 of the spectrometer 120 generate an intensity 141versus wavelength 143, e.g., a spectrum 147 on a display screen 140. Asshown in FIG. 3 , the spectrometer 120 generates a spectrum data 152,which includes intensity 141 per wavelength 143 of the received beams oflight by the lens 122 and detected by the light detectors 121.

As shown in FIG. 3 , the beam of light 146 that has the wavelength w3focuses on the substrate 130, e.g., at the bottom of the dip 133 of thesubstrate 130. In addition, the deflected beam of light 146 impinging onthe pinhole structure 124 also focuses on the pinhole structure 124 andentirely passes through the pinhole 149 and thus produces a peakintensity in the light detectors 121. Also, the spectrum 147 produces apeak at the wavelength w3 of the beam of light 146.

As shown in FIG. 3 , the reflected light from the surface 131 of thesubstrate 130 is received by the optical device 114 and is deflected bythe optical device 114 to the pinhole structure 124. As shown the beamof lights 142 and 144, having the wavelengths w1 and w2, e.g., violetand green lights, do not focus on the surface 131 of the substrate 130.The beam of light 146, having the wavelength w3, e.g., the red light,focuses on a bottom surface of the dip 133 in the substrate 130. Thus,the reflected light from the red beam of light also focuses at thepinhole 149 and entirely passes through the pinhole 149. Thus, theintensity versus wavelength, e.g., the spectrum 147, has a peak in thered region. In some embodiments the wavelength of the peak intensity inthe red region determines that a depth 155 of the dip 133 is about 5microns.

FIGS. 4A and 4B illustrate substrates that include scratches inaccordance with some embodiments of the present disclosure. FIG. 4Ashows a backside 408 of a substrate 400 with scratches and particlesthat includes a bump 404 and a dip 402. In some embodiments, the bump404 on the backside 408 of the substrate is caused by or may cause a dip(not shown) on the front side 415 of the substrate. In some embodiments,the dip 402 on the backside 408 of the substrate is caused by or maycause a bump 406 on the front side 415 of the substrate. In someembodiments, the backside 408 of a substrate 400 is scanned by theoptical scanning systems 100, 200, or 300 of FIGS. 1-3 . In someembodiments, the bump 404 is scanned along a direction 412 that isparallel to a Y-direction 410 and the dip 402 is scanned along adirection 414 that is parallel to an X-direction 420. In someembodiments, a scratch on the backside 408 of the substrate 400, e.g.,the dip 402 or the bump 404, does not have an associated scratch on thefront side 415 of the substrate 400, however, the scratch on thebackside 408 of the substrate 400 may cause a defect or wafer printingerror in the thickness 413 of the substrate 400. Thus, the backside 408and the front side 415 of the substrate 400 is scanned in someembodiments. In some embodiments, an edge region is a region extending10 percent of the width of the substrate 400 in the X-direction andextending 10 percent of the length of the substrate 400 in theY-direction. The substrate 400 is more vulnerable to having thescratches in the edge region and the bump 404 and the dip 402 may be inthe edge region of the substrate 400. In some embodiments, the bump hasa height of about 5 microns to about 15 microns, e.g., 10 microns.

FIG. 4B shows a backside surface 458 of a substrate 450 with scratchesthat includes bumps 452, 454, 466, 468; and dips 462, 464, and 470. Asshown, the dip 462 on the backside surface 458 of the substrate 450 iscaused by or may cause a bump 456 on the front side 455 of the substrate450. In some embodiments, the backside surface 458 of a substrate 450 isscanned by the optical scanning systems 100, 200, or 300 of FIGS. 1-3 .In some embodiments, the dip 464 follows the bump 454 in a direction 451that is parallel to the Y-direction 410 and the dip 462 follows the bump452 in a direction 453 that is parallel to the X-direction 420. In someembodiments, the bump 454 and the dip 464 are scanned along thedirection 451 and the bump 452 and the dip 462 are scanned along thedirection 453. In some embodiments, an entire backside of the substrate450 including the bumps 452, 454, 466, 468 and the dips 462, 464, and470 are scanned either along multiple parallel lines parallel to theY-direction, along multiple parallel lines parallel to the X-direction,or both. In some embodiments, the edge region of the backside of thesubstrate 450 is scanned.

FIG. 5 illustrates a detector systems for the optical scanning system inaccordance with some embodiments of the present disclosure. FIG. 5 showsthe detector system 500 that includes the spectrometer 120, whichreceives the beams of light 510 through the lens 122. As described, thespectrometer 120 includes a prism for splitting the direction oftransmission of the multiple wavelengths and thus directing eachwavelength, e.g., a short wavelength range, to one of the lightdetectors 121 of the spectrometer 120. In some embodiments, each lightdetector 121 of the spectrometer 120 includes a filter for selecting aspecific wavelength, a specific short wavelength range, of the beam oflight 510. The output of the spectrometer 120 is the spectrum data 152,which includes intensity 141 per wavelength 143 of the received beams oflight 510. The detector system 500 also includes a peak detector 502,consistent with the peak-wavelength detector 125 of FIGS. 1A, 1B, 2, and3 , that receives the spectrum data 152 and generates a peak wavelength154 of the spectrum data 152 corresponding to the peak intensity of thespectrum data 152. Thus, the peak intensity of the spectrum data 152 isat the peak wavelength 154.

The detector system 500 also includes a peak threshold verifier 504 thatreceives the spectrum data 152 and the peak wavelength 154 having thepeak intensity. The peak threshold verifier 504 may further determine anaverage value of the spectrum data and a shape of the spectrum data 152around the peak intensity. The peak threshold verifier 504 verifies thepeak intensity at the peak wavelength 154. In some embodiments, the peakintensity at the peak wavelength 154 in addition to being the peak valueof the spectrum data 152, is at least two times greater than the averagevalue of the spectrum data 152. In some embodiments, the shape of thespectrum data 152 around the peak intensity is a bump protruding outwardand the peak threshold verifier 504 verifies that bump has a widthwithin a threshold range. After verifying the peak wavelength 154, thepeak wavelength 154 is inputted to the wavelength-to-height converter126. In some embodiments, the wavelength-to-height converter 126determines the associated height 156 of the surface 131 of the substrate130 based on the peak wavelength 154. In some embodiments, thepeak-wavelength detector 125 of FIGS. 1A, 1B, 2, and 3 , is consistentwith the combination of the peak detector 502 and the peak thresholdverifier 504.

As noted, based on the height of the substrate, a specific wavelengthconverges, e.g., focuses, on the surface 131 of the substrate 130. Asdescribed above and shown in FIG. 1A, the beam of light 144 having thewavelength w2 converges on the bump 132 when the stage 112 is at alocation, e.g., position, that the bump 132 is illuminated by theoptical device 114. As noted, when the wavelength w2 converges on thebump 132, the deflected beam of light 144 entirely passes through thepinhole 149 and thus the peak of the spectrum data 152 is at wavelengthw2, which is the peak wavelength.

In addition, as described above and shown in FIG. 3 , the beam of light146 having the wavelength w3 converges at the bottom of the dip 133 whenthe stage 112 is at a location that the dip 133 is illuminated by theoptical device 114. When the wavelength w3 converges at the bottom ofthe dip 133, the deflected beam of light 146 entirely passes through thepinhole 149 and thus the peak of the spectrum data 152 is at wavelengthw3. Thus, based on the peak wavelength 154 the height 156 at the surface131 of the substrate 130 is determined.

Thus, the height of the surface 131, e.g., the height 145 of the bump132, is determined based on the wavelength w2 and the height of thesurface 131, a depth at the bottom of the dip 133, is determined basedon the wavelength w3. In some embodiments, the location of the stage 112is provided by the stage controller 110. Thus, for each location of thestage 112, e.g., a corresponding location 158 of the surface 131 of thesubstrate 130, the height 156 at the surface 131 of the substrate 130 isdetermined by the wavelength-to-height converter 126. In someembodiments, a height-vs-location identifier 128 receives a location 158of the surface 131 of the substrate 130 as well as the height 156 at thesurface 131 of the substrate 130 for multiple points of the surface 131of the substrate 130 and provides a line scan data 161, e.g., a mapdata, of the height of the surface 131 of the substrate 130.

FIGS. 6A and 6B illustrate line scans through the substrates of FIG. 4Athat include scratches and particle in accordance with some embodimentsof the present disclosure. As shown in FIG. 6A, a graph 600, e.g., aprofile, shows a line scan of the backside 408 of the substrate 400having the bump 404 over the backside surface. In some embodiments, thehorizontal coordinate is along the scanning direction 412 and is inmillimeter and the vertical coordinate 604 is the height of the surfaceof the substrate 130 and is in microns. The backside surface of thesubstrate is displayed with an initial height 608. The bump 404 has amaximum height 630, where the maximum height is at location 636 on thehorizontal coordinate that is along the direction 412 of FIG. 4A. Themaximum height 630 is above the initial height 608 by a distance 634. Insome embodiments, the distance 634 is between 2 microns and 15 microns,e.g., 10 microns. In some embodiments, the height 630 corresponds towavelength w2.

As shown in FIG. 6B, a graph 610, e.g., a profile, shows a line scan ofthe backside 408 of the substrate 400 having the dip 402 over thebackside surface. The backside surface of the substrate is displayedwith an initial height 618. The dip 402 has a maximum depth 632, wherethe maximum depth 632 is at location 638 on the horizontal coordinatethat is along the scanning direction 414 of FIG. 4A. The maximum depth632 is below the initial height 618 by a distance 635. In someembodiments, the distance 635 is between 2 microns and 10 microns, e.g.,5 microns. In some embodiments, the graphs 600 and 610 are generated bythe optical scanning system 100, 200, or 300 of FIGS. 1-3 . In someembodiments, the depth 632 corresponds to wavelength w3.

FIGS. 7A and 7B illustrate line scans through the substrates of FIG. 4Bthat include scratches and particle in accordance with some embodimentsof the present disclosure. As shown in FIG. 7A, a graph 700, e.g., aprofile, shows a line scan of the backside surface 458 of the substrate450 having the bump 454 and the dip 464 over the backside surface 458.In some embodiments, the horizontal coordinate is along the scanningdirection 451 and the vertical coordinate 604 is the height. Thebackside surface of the substrate is displayed with an initial height725. The graph 700 shows that the backside scan has a bump around adistance 712 with a maximum height 722 at the distance 712. The graph700 also shows that the backside scan has a dip around a distance 714with a minimum height 724 at the distance 714. In some embodiments, theinitial height 725 of the surface 131 of the substrate 130 correspondsto locations of the surface 131 of the substrate 130 which has no bumpsor dips. In some embodiments, the maximum height 722 has a distance 726above the initial height 725 and the minimum height 724 has a distance728 below the initial height 725. In some embodiments, the maximumheight 722 corresponds to the wavelength w2 and the minimum height 724corresponds to the wavelength w3.

As shown in FIG. 7B, a graph 710, e.g., a profile, shows a line scan ofthe backside surface 458 of the substrate 450 having the bump 452 andthe dip 462 over the backside surface 458. In some embodiments, thehorizontal coordinate is along the scanning direction 453 and thevertical coordinate 604 is the height. The backside surface of thesubstrate is displayed with the initial height 725. The graph 710 showsthat the backside scan has a bump around a distance 716 with a maximumheight above the height 722 at the distance 716. The graph 710 alsoshows that the backside scan has two dips around distances 715 and 717with two minimum depth below the height 724. In some embodiments, theinitial height 725 of the surface 131 of the substrate 130 correspondsto locations of the surface 131 of the substrate 130 which has no bumpsor dips. In some embodiments, the height 722 corresponds to thewavelength w2 and the height 724 corresponds to the wavelength w3. Insome embodiments, the maximum of the bump 452 corresponds to thewavelength w1. In some embodiments the maximum height of the bump 452 isbetween 10 microns and 20 microns, e.g., 15 microns.

FIG. 8 illustrates an exemplary optical scanning system 800 fordetermining scratches including bumps and/or dips of a substrate inaccordance with some embodiments of the disclosure. The optical scanningsystem 800 includes an analyzer module 830 and a main controller 840coupled to each other. Referring back to FIG. 1 or 3 , the analyzermodule 830 receives the wavelength 154 of the peak intensity of thespectrum data 152 of the reflected light from the surface of thesubstrate and determines, e.g., calculates, a height 156 of the surfaceof the substrate based on the received wavelength 154. The analyzermodule 830 receives the wavelength 154 of the peak intensity from a peakdetector 810, which is consistent with the peak-wavelength detector 125of FIGS. 1A and 1 s also consistent with a combination of the peakdetector 502 and the peak threshold verifier 504. The peak detector 810is either directly coupled to the analyzer module 830 or is coupled tothe analyzer module 830 via the main controller 840.

In some embodiments, the analyzer module 830 is consistent with acombination of the peak-wavelength detector 125 and thewavelength-to-height converter 126 of FIGS. 1A, 1B, 2, and 3 . As shownin FIG. 8 , the main controller 840, controls the other controllers,devices, and systems. In some embodiments, a main controller (notshown), consistent with the main controller 840, controls the timing andfunctionality of the optical controller 118, light source controller135, the spectrometer 120, the stage controller 110 and the displaycontroller 115 of the optical scanning systems 100 and 300 of FIGS. 1Aand 3 . The main controller enables the optical scanning systems 100 or300 to scan a surface of the substrate 130 and display a map of thespecific range of heights on the surface of the substrate as shown inFIGS. 7A and 7B. In some embodiments, a main controller (not shown),consistent with the main controller 840, controls the timing andfunctionality of the optical controller 118, the spectrometer 120, thestage controller 110, the display controller 115, and the optical system185 (via the optical controller 118) of the optical scanning system 180of FIG. 1B.

In some embodiments, the main controller 840 is coupled to a lightsource controller 808, a display controller 806, an optical controller804, and a stage controller 802. In some embodiments and returning backto FIG. 1A the optical controller 804 is consistent with the opticalcontroller 118. The optical controller 804, which is controlled by themain controller 840, controls the optical device 114 to performtransmitting a converging beam of light to the surface of the substrate,receiving the reflected light from the surface of the substrate, andtransmitting the reflected light from the surface of the substrate tothe pinhole structure 124. In addition, the optical controller 804 maycontrol a location of the pinhole structure 124 and a size of thepinhole 149 such that the beam of light having the wavelength thatfocuses on the surface of the substrate focuses at the pinhole structure124 and passes, e.g., entirely passes, through the pinhole 149 and theother beams of light having other wavelengths do not pass through thepinhole 149 or a fraction passes through the pinhole 149. The opticalcontroller 804 also controls the light source controller 808, which isconsistent with the light source controller 135 of FIG. 1A, to controlthe light source 116 and to generate the beam of light 134 that includesa plurality of wavelengths to transmit the beam of light 134 to theoptical device 114.

In some embodiments, the main controller 840 is coupled to and controlsthe stage controller 802, which is consistent with the stage controller110 of FIG. 1A, to move the substrate such that the optical device 114receives the reflected light from different points on the surface of thesubstrate. In some embodiments, the main controller 840 is coupled toand controls the display controller 806, which is consistent with thedisplay controller 115 of FIG. 1A, to display a spectrum of thereflected beam of light from a location of the substrate on the displayscreen 140 or to display a scan line of the height of the surface of thesubstrate on the display screen 140.

FIG. 9 illustrates a flow diagram of an exemplary process for scanning asubstrate and determining scratches including bumps and/or dips of thesubstrate in accordance with some embodiments of the disclosure. Theprocess 900 may be performed by the optical scanning system of FIGS. 1,2, 4, and 8 . In some embodiments, the process 900 or a portion of theprocess 900 is performed and/or is controlled by the computer system1000 described below with respect to FIGS. 10A and 10B. The methodincludes the operation S902 of transmitting a converging beam of lightthat comprises multiple wavelengths to a substrate. As shown in FIG. 1A,the beam of light 134 is transmitted by the light source 116 and thebeam of light 134 is focused by the optical device 114. In operationS904, reflected light from the surface of the substrate is received. Asshown in FIG. 1A, the reflected light is received by the spectrometer120. In operation S906, a height or depth of the surface of thesubstrate is determined based on a wavelength of the reflected light. Asdiscussed, the height or depth is determined based on the wavelengthcorresponding to the peak intensity of the detected light from thesurface of the substrate. In some embodiments and referring back to FIG.1A, the analyzer module 830 of FIG. 8 determines the wavelength of thepeak intensity of the spectrum data 152 and also determines the heightof the surface 131 of the substrate 130 based on the determinedwavelength.

FIGS. 10A and 10B illustrate an apparatus for scanning a substrate anddetermining scratches including bumps and dips of the substrate inaccordance with some embodiments of the disclosure. FIG. 10A is aschematic view of a computer system 1000 that executes the process fordetermining the bumps and dips of the substrate according to one or moreembodiments as described above. All of or a part of the processes,method and/or operations of the foregoing embodiments can be realizedusing computer hardware and computer programs executed thereon. Theoperations include converging a multi-wavelength beam of light on asubstrate for determining bumps and dips of the substrate. Thus, in someembodiments, the computer system 1000 provides the functionality of theoptical controller 804, the analyzer module 830, the main controller840, the stage controller 802, the light source controller 808, the peakdetector 810, and the display controller 806. In FIG. 10A, a computersystem 1000 is provided with a computer 1001 including an optical diskread only memory (e.g., CD-ROM or DVD-ROM) drive 1005 and a magneticdisk drive 1006, a keyboard 1002, a mouse 1003, and a monitor 1004. Insome embodiments, the computer system 1000 provides the functionality ofthe optical controller 118, the light source controller 135, the stagecontroller 110, and the display controller 115 of FIG. 1A. As described,in some embodiments, a main controller, consistent with the maincontroller 840, controls the timing and functionality the othercontrollers, devices, and systems of the optical scanning systems ofFIGS. 1A, 1B, 2, and 3 . Thus, the computer system 1000 also providesthe functionality of the main controller.

FIG. 10B is a diagram showing an internal configuration of the computersystem 1000. In FIG. 10B, the computer 1001 is provided with, inaddition to the optical disk drive 1005 and the magnetic disk drive1006, one or more processors 1011, such as a micro-processor unit (MPU),a ROM 1012 in which a program such as a boot up program is stored, arandom access memory (RAM) 1013 that is connected to the processors 1011and in which a command of an application program is temporarily storedand a temporary storage area is provided, a hard disk 1014 in which anapplication program, a system program, and data are stored, and a bus1015 that connects the processors 1011, the ROM 1012, and the like. Notethat the computer 1001 may include a network card (not shown) forproviding a connection to a LAN.

The program for causing the computer system 1000 to execute the processfor determining the scratches including bumps and/or dips of thesubstrate in the foregoing embodiments may be stored in an optical disk1021 or a magnetic disk 1022, which are inserted into the optical diskdrive 1005 or the magnetic disk drive 1006, and transmitted to the harddisk 1014. Alternatively, the program may be transmitted via a network(not shown) to the computer 1001 and stored in the hard disk 1014. Atthe time of execution, the program is loaded into the RAM 1013. Theprogram may be loaded from the optical disk 1021 or the magnetic disk1022, or directly from a network. The program does not necessarily haveto include, for example, an operating system (OS) or a third partyprogram to cause the computer 1001 to execute the process formanufacturing the lithographic mask of a semiconductor device in theforegoing embodiments. The program may only include a command portion tocall an appropriate function (module) in a controlled mode and obtaindesired results.

In some embodiments, implementing the processes and methods mentionedabove, increases the throughput of scanning the backside of a substratesuch a mask blank. In processes of manufacturing an integrated circuitor a die by EUV lithography process, a substrate, e.g., a mask blank, abackside of a mask or a patterned mask, is scanned for bumps and dipsbefore the lithography process. When detecting a unwanted bump or dip onthe mask and imaging a layout pattern on the mask blank by the presentdisclosure, the mask or region with bumps and dips can be effectivelyavoided or repaired for wafer printing error concerns. Accordingly, themask used in the EUV lithography process is qualified by the system andmethod of the present disclosure.

It will be understood that not all advantages have been necessarilydiscussed herein, no particular advantage is required for allembodiments or examples, and other embodiments or examples may offerdifferent advantages.

According to some embodiments of the present disclosure, a method ofscanning a substrate includes transmitting a converging beam of lightthat comprises multiple wavelengths to the substrate. Each wavelength ofthe multiple wavelengths focuses at a different distance in a focusinterval around and including a surface of the substrate. The methodalso includes receiving reflected light from the surface of thesubstrate and determining a height or depth of the surface of thesubstrate based on a wavelength of the reflected light having a highestintensity. In an embodiment, the method further includes irradiating thesurface of the substrate with the converging beam of light from a lightsource located at a first distance from the surface of the substrate.The surface of the substrate is a backside surface of the substrate andthe light source is located above the backside surface of the substrate.In an embodiment, the first distance is a perpendicular distance betweenthe light source and a flat portion of the surface of the substrate withno bumps or dips. In an embodiment, the surface of the substrateincludes one or more of bumps and dips, wherein a height of a bump or adepth of dip on the surface of the substrate is determined with respectan area having with no bumps or dips surrounding the bump or the dip. Inan embodiment, the reflected light from the surface of the substrate isreceived by a spectrometer, the method further includes detecting thereflected light from a first point on the surface of the substrate,determining a spectrum of the detected reflected light, determining afirst wavelength of a peak intensity of the spectrum, and determiningthe height or depth of the first point on the surface of the substratebased on the first wavelength of the peak intensity. In an embodiment,the spectrometer includes a lens at an input to the spectrometer. Thelens focuses the reflected light from the surface of the substrate ontoone or more light detectors and each light detector includes a filter toselect a specific wavelength range to generate a signal proportional toan intensity of the reflected light in the specific wavelength range. Inan embodiment, a portion of the converging beam of light having thefirst wavelength is configured to focuses on the surface of thesubstrate. In an embodiment, a pinhole structure having a pinhole isarranged before the lens of the spectrometer. The reflected light withthe first wavelength focuses on the pinhole structure and the reflectedlight with the first wavelength substantially entirely passes throughthe pinhole. In an embodiment, the reflected light having one or morewavelengths other than the first wavelength does not focus on thepinhole. In an embodiment, a fraction of the reflected light passesthrough the pinhole when the reflected light has the other than thefirst wavelength. In an embodiment, the reflected light having awavelength that does not focus on the surface of the substrate does notfocus on the pinhole structure. In an embodiment, the substrate isarranged on a stage and the method further includes configuring thestage to move the substrate in a first direction and receiving thereflected light from the surface of the substrate at one or moredifferent points along the first direction, scanning the surface of thesubstrate by the converging beam of light, receiving the reflected lightfrom the surface of the substrate in a specific range of wavelengthscorresponding to a specific range of heights, and determining a map ofthe specific range of heights on the surface of the substrate on a scanline along the first direction. In an embodiment, the method furtherincludes moving the stage in parallel lines along the first direction ormoving the stage in parallel lines perpendicular to the first directionto scan the substrate, receiving the reflected light from the surface ofthe substrate in a specific range of wavelength corresponding to aspecific range of heights, and determining a map of the specific rangeof heights on the surface of the substrate. In an embodiment, the lightsource is a white light source and the multiple wavelengths are in whitelight spectrum.

According to some embodiments of the present disclosure, a method ofscanning a substrate includes receiving reflected light from a firstpoint on a surface of the substrate and configuring the reflected lightto pass through a pinhole. The method includes detecting the reflectedlight from the first point after passing the pinhole and determining aspectrum of the detected reflected light. The method also includesdetermining a first wavelength of a peak intensity of the spectrum anddetermining a height or depth of the first point on the surface of thesubstrate based on the first wavelength of the peak intensity. In anembodiment, the substrate is arranged on a stage and the method furtherincludes configuring the stage to move the substrate in a firstdirection and receiving the reflected light from the surface of thesubstrate at one or more different points along the first direction,scanning the surface of the substrate by a converging beam of light,receiving the reflected light from the surface of the substrate in aspecific range of wavelength corresponding to a specific range ofheights, and determining a map of the specific range of heights on thesurface of the substrate on a scan line along the first direction.

According to some embodiments of the present disclosure, a system forscanning a substrate includes a main controller, a light source coupledto the main controller and to transmit a beam of light that includesmultiple wavelengths to the substrate, and a stage coupled to the maincontroller and configured to move the substrate. The system alsoincludes an optical system disposed in a light path between the lightsource and the substrate and coupled to the main controller andconfigured for focusing the beam of light on a surface of the substrate,and a spectrometer to receive the beam of light reflected from thesurface of the substrate and directed by the optical system andconfigured for detecting reflected light from a first point on thesurface of the substrate, determining a spectrum of the detectedreflected light determining a first wavelength of a peak intensity ofthe spectrum, and determining a height or depth of the first point onthe surface of the substrate based on the first wavelength of the peakintensity. In an embodiment, the spectrometer includes a lens forfocusing the reflected light onto the one or more light detectors. Eachlight detector generates a signal proportional to the reflected light ina specific wavelength range. In an embodiment, the light source is awhite light source and the multiple wavelengths are in white lightspectrum. In an embodiment, the system further includes a pinholedisposed in a light path between the substrate and the spectrometer. Thepinhole is arranged before the lens of the spectrometer, the reflectedlight with the first wavelength focuses on the pinhole and substantiallyentirely pass through the pinhole, and the reflected light havingwavelengths other than the first wavelength does not focus on thepinhole and a fraction of the reflected light passes through the pinholewhen the reflected light has other than the first wavelength.

The foregoing outlines features of several embodiments or examples sothat those skilled in the art may better understand the aspects of thepresent disclosure. Those skilled in the art should appreciate that theymay readily use the present disclosure as a basis for designing ormodifying other processes and structures for carrying out the samepurposes and/or achieving the same advantages of the embodiments orexamples introduced herein. Those skilled in the art should also realizethat such equivalent constructions do not depart from the spirit andscope of the present disclosure, and that they may make various changes,substitutions, and alterations herein without departing from the spiritand scope of the present disclosure.

What is claimed is:
 1. A method of scanning a substrate, comprising:transmitting a converging beam of light that comprises multiplewavelengths to a back surface of the substrate, wherein each wavelengthof the multiple wavelengths is configured to focus at a differentdistance in a focus interval around and including the back surface ofthe substrate; receiving reflected light bounced back from the backsurface of the substrate; determining, based on a spectrum of thereflected light intensity versus wavelength, a first wavelength of thereflected light having a highest intensity, wherein the highestintensity is verified to be a peak intensity if the highest intensity isat least two times greater than an average intensity value of thespectrum, and wherein the converging beam with the first wavelengthfocuses at a first location; and determining a height or depth at thefirst location from the back surface of the substrate directly and onlybased on the first wavelength of the reflected light as a peakwavelength corresponding to the peak intensity.
 2. The method of claim1, further comprising: before transmitting the converging beam of light,placing the substrate on a stage such that a front surface faces thestage.
 3. The method of claim 1, wherein the multiple wavelengthsrespectively focus at the first location on the back surface of thesubstrate and without entering the substrate and get reflected from thefirst location, focus above the first location and without entering thesubstrate and get reflected from the first location of the back surfaceof the substrate, and get reflected from the first location of the backsurface of the substrate without being focused and without entering thesubstrate.
 4. The method of claim 1, further comprising irradiating theback surface of the substrate with the converging beam of light from alight source located at a first distance from the back surface of thesubstrate, wherein a beam splitter is disposed between the light sourceand the stage such that the beam of light from the light source passesthrough the beam splitter.
 5. The method of claim 4, wherein the firstdistance is a perpendicular distance between the light source and a flatportion of the back surface of the substrate with no bumps or dips. 6.The method of claim 4, wherein the reflected light bounced back from theback surface of the substrate is received by a spectrometer.
 7. Themethod of claim 6, further comprises: detecting the reflected lightbounced back from the first location by the spectrometer; determiningthe spectrum of the detected bounced back reflected light by thespectrometer; determining the first wavelength as a wavelength at thepeak intensity of the spectrum; and determining the height or depth ofthe first location based on the first wavelength of the peak intensityof the spectrum.
 8. The method of claim 6, wherein the spectrometercomprises a lens at an input to the spectrometer, the lens is configuredto focus the reflected light bounced back from the back surface of thesubstrate onto one or more light detectors, and wherein each lightdetector comprises a filter to select a specific wavelength range and togenerate a signal proportional to an intensity of the reflected light inthe specific wavelength range.
 9. The method of claim 8, wherein apinhole structure having a pinhole is arranged before the lens of thespectrometer, wherein the reflected light is deflected by the beamsplitter at about 90 degrees and is directed to the pinhole structure.10. The method of claim 9, wherein the reflected light with the firstwavelength is configured to focus at the pinhole and substantiallyentirely passes through the pinhole, and wherein the reflected lighthaving one or more wavelengths other than the first wavelength isconfigured not to focus on the pinhole.
 11. A method of scanning asubstrate, comprising: receiving reflected light bounced back based onan incident light directed at a first location of a surface of thesubstrate, the first location including a defect; determining a spectrumof the detected reflected light intensity versus wavelength; determininga first wavelength of a peak intensity of the spectrum, wherein ahighest intensity of the spectrum is verified to be the peak intensityif the highest intensity is at least two times greater than an averageintensity value of the spectrum, and wherein the incident light with thefirst wavelength focuses at the first location; and determining a heightor a depth of the defect measured from the open surface of the substratedirectly and only based on the first wavelength as a peak wavelengthcorresponding to the peak intensity.
 12. The method of claim 11, furthercomprising: configuring the reflected light to pass through a pinhole;and detecting the reflected light bounced back from the first locationafter passing through the pinhole.
 13. The method of claim 11, whereinthe substrate is arranged on a stage, the method further comprising:configuring the stage to move the substrate in a first direction andreceiving the reflected light bounced back from the open surface of thesubstrate at one or more different locations along the first direction;scanning the open surface of the substrate by a converging beam oflight; receiving the reflected light bounced back from the open surfaceof the substrate in a specific range of wavelengths corresponding to aspecific range of heights and depths on the open surface of thesubstrate; and determining a map of the specific range of heights anddepths on the open surface of the substrate on a scan line along thefirst direction.
 14. The method of claim 11, wherein the defectcomprises one or more of bumps and dips, wherein a height of a bump anda depth of a dip measured from the open surface of the substrate isdetermined with respect an area having with no bumps or dips surroundingthe bump or the dip.
 15. The method of claim 11, wherein the reflectedlight comprises multiple wavelengths in white light spectrum, the methodfurther comprising: deflecting the reflected light at about 90 degreesto be directed at the pinhole, wherein a portion of the reflected lightwith the first wavelength focuses at the pinhole and substantiallyentirely passes through the pinhole.
 16. The method of claim 11, whereinthe incident light is bounced back by roughness at the first locationwithout entering the substrate.
 17. A system for scanning a substrate,comprising: an optical system disposed in a light path between a lightsource and the substrate and coupled to a main controller and configuredfor focusing a beam of light transmitted from the light source on anopen surface of the substrate; and a spectrometer to receive a reflectedbeam of light bounced back by roughness on the open surface of thesubstrate, wherein the reflected beam of light is directed by theoptical system to the spectrometer, the spectrometer is configured for:detecting reflected light bounced back from a first location including adefect on the open surface of the substrate; determining a spectrum ofthe detected reflected light intensity versus wavelength; determining afirst wavelength of a peak intensity of the spectrum, wherein the peakintensity of the spectrum is defined to be at least two times greaterthan an average intensity value of the spectrum; and determining aheight or a depth of the defect measured from the open surface of thesubstrate directly and only based on the first wavelength as a peakwavelength corresponding to the peak intensity.
 18. The system of claim17, wherein the light source is a white light source and the multiplewavelengths are in white light spectrum.
 19. The system of claim 17,wherein the spectrometer includes a lens configured for focusing thereflected light onto one or more light detectors of the spectrometer,and wherein each light detector is configured to generate a signalproportional to the reflected light in a specific wavelength range. 20.The system of claim 19, further comprising a pinhole disposed in a lightpath between the substrate and the spectrometer, wherein the pinhole isarranged before the lens of the spectrometer, wherein the reflectedlight is deflected at about 90 degrees to be directed to thespectrometer and the reflected light having the first wavelength isconfigured to focus on the pinhole and substantially entirely passthrough the pinhole to reach a first light detector, and wherein thereflected light having wavelengths other than the first wavelength isconfigured to not focus on the pinhole and a fraction of the reflectedlight having the wavelengths other than the first wavelength to passthrough the pinhole to reach the first light detector.